1. Models of Yukawa interaction in the two Higgs doublet model, and their collider phenomenology Kei Yagyu Univ. Toyama Collaborators Mayumi Aoki, Shinya Kanemura, Koji Tsumura arXiv:0902.4665 [hep-ph] April 20 TILC09 @Tsukuba, Japan

2. Possibility of extended Higgs models Higgs boson has not been discovered. →Various possibilities for extended Higgs sector Problems which cannot be explained in the SM →Need to go the beyond SM →Extended Higgs models appear in low energy effective theories Extended Higgs models New physics ・ Hierarchy problem ・ Tiny neutrino mass ・ Dark matter ・ Baryon asymmetry of Universe

3. Two basic constraints from the experimental data ① Electroweak precision measurements (LEP) ② To avoid tree-level FCNC Multi Higgs doublets (+ singlets) dd

4. Two basic constraints from the experimental data ① Electroweak precision measurements (LEP) ② To avoid tree-level FCNC dd Multi Higgs doublets (+ singlets) GIM mechanism Discrete Z 2 symmetry

5. Two-Higgs-Doublet Model (THDM) ・ Simplest extended Higgs model ・ SM ： Φ 1 THDM ： Φ 1, Φ 2 ・ Physical states ： H SM h, H, A, H ± MSSM, NMSSM, etc… Possible models of DSB THDM Radiative neutrino mass model So, it would be valuable to study collider phenomenology of THDM. ・ m ν ・ m ν + DM ・ m ν + DM + B Zee, Phys Lett.B 93 (1980) Ma, PRD 73 (2006) Aoki, Kanemura, Seto PRL 102 (2009) Holdom arXiv/0606146

6. Higgs potential under the discrete symmetry ChargedCP-evenCP-odd ↑ Higgs mechanism Physical degrees of freedom ： 8-3=5 H ±, A, H, h The physical states are defined by the mixing angles α and β. The ratio of vevs is defined by And the soft breaking mass parameter is..

7. Type of Yukawa interaction in THDM Four types of Yukawa interactions under the discrete symmetry (to avoid FCNC) ・ Type-II THDM: MSSM Φ 1 couples to down-type quarks and leptons. Φ 2 couples to up-type quarks. b→sγ bound is very strong Light H + is forbidden ・ Type-X THDM : AKS model Φ 1 couples to leptons Φ 2 couples to quarks b→sγ bound is mild Light H + is possible ! In this talk, we mainly discuss the Type-X THDM and the MSSM Barger, Hewett, Phillips PRD 41 (1990) Grossman NPB 426 (1994)

8. m H+ ＞ 295GeV [95% C.L.] (Type-II,Y) No bound (Type-I ， -X) :1σ :2σ NLO b→sγ NLO calculation Ciuchini et al.Nucl. Phys. B 527, 21 (1998). NNLO calculation Misiak, Steinhauser, Nucl. Phys. B 764, 62 (2007). Misiak et al., PRL. 98, 022002 (2007). Light charged Higgs are possible in the Type-X and MSSM Aoki, Kanemura, Tsumura, K.Y arXiv:0902.4665 [hep-ph]

9. A decays Type-I, -II, -Y → bb, Type-X → τ + τ - (Also H decays when sin(β-α)=1 ) BR(A → X) 10 -3 10 -1 10 -2 1 m A =m H+ =150GeV

10. H + decays Type-I, -II, -X → τν, Type-Y → cb (hadron jets) BR(H + → X) 10 -3 10 -1 10 -2 1 m A =m H+ =150GeV

11. Discrimination between models in the light charged Higgs scenario at the LHC Scenario m A =m H =m H+ :130~150GeV sin(β-α)=1 M~ m A =m H =m H+ Single A/H production at the LHC Higgs pair production (AH +, HH + ) at the LHC |δρ|<10 -3 Custodial symmetry exists,and perturbative unitarity is satisfied with this condition. m H + =300 GeV sin(β-α)=1

12. Single A/H production at the LHC (30fb -1 ) gg→A/H→ τ + τ - pp→bbA/H → bb τ + τ - (ATLAS TDR) Signal (after the cut) ： 49 Background (after the cut) W+jet: 46 tt: 6 bb: 29 Z/γ*: 5 Sum: 86 Signal (after the cut) ： 72 Background (after the cut) W+jet: 530 tt: 7 bb: 14 Z/γ*: 163 Sum: 714 Kinematical cuts ・ A veto against b-jets for p T >15GeV and η<2.5. ・ τ τ’s invariant mass cut. m ττ -1.5σ<m ττ < m ττ +1.5σ σ~27GeV tanβ=10, m A =150GeV, MSSM Kinematical cuts ・ At least one tagged b-jet. ・ At most two non-b jets with p T >15GeV and η<3.2. ・ τ τ’s invariant mass cut. m ττ -1.5σ<m ττ < m ττ +1.5σ σ~39GeV

13. Significance (S/root(B)) gg→τ + τ - pp→bbτ + τ - Aoki, Kanemura, Tsumura, K.Y arXiv:0902.4665 [hep-ph] MSSM Type-X High tanβMid tanβLow tanβ Direct Associate

14. AH + (HH + ) production at the LHC (300fb -1 ) BR(H + →τ + ν) ～ 100% BR(H→τ + τ - ) ～ 100% ~30000 events ～ 7pb BR(W + →τ + ν) ～ 10% BR(Z→τ + τ - ) ～ 3% ~6300 events bbτν final states τττν final states σ(ud→HH + ) ～ 100fb 30000 AH + (HH + ) events at 300fb -1 bbτν→MSSM (Type-II) τττν→Type-X In the MSSM taking kinematical cuts there is possibility to detect this final states. detailed analysis: Cao, Kanemura, Yuan hep-ph/0402226

15. Physics of the Type-X THDM at the ILC

16. Discrimination of the models at the ILC m A =m H =150GeV, sin(β-α)=1, tanβ=10 and root(s)=500GeV Type-X branching ratio of leptonic decay is much larger than Type-II one. The ττμμ and ττττ mode are valuable to study the Type-X Yukawa interaction. Type-IIType-X BR (A/H→ττ)0.1050.995 BR (A/H→μμ)O (10 -4 )0.003 150 30

17. Signal background analysis for ττμμ events For L=500fb -1 After invariant mass cuts S~96 B~9 M μμ [GeV] dσ/dM μμ [pb/GeV] M μμ [GeV] dσ/dM μμ [pb/GeV] The μμ invariant mass distribution Taking kinematical cuts we can obtain S/Sqrt(S+B) ~ 9 mZmZ A/H Signal !

18. Signal background analysis for ττ ττ events The ττ invariant mass distribution dσ/dM μμ [pb/GeV] mZmZ M ττ [GeV] For L=500fb -1 After cuts S~7350 B~41 A/H Signal ! Taking kinematical cuts we can obtain S/Sqrt(S+B) ~ 85 !! But we assumed that tau tagging efficiency is 100% → Realistic simulation study is necessary.

19. Summary of the model discrimination in the light H ± scenario SM THDM low tanβ Type-X high tanβ MSSM Mid tanβ b-jet signal →MSSM Leptonic signal→Type-X H ± discovery Top-quark decay AH +, HH +, AH production 300fb -1 @ LHC, 500fb -1 @ ILC Single A/H production 30fb -1 @ LHC m H+ <m t -m b

20. Summary In the THDM, there are four types of Yukawa interaction under the discrete symmetry to avoid tree-level FCNC. The Type-II THDM corresponds to the MSSM Yukawa interaction, while the Type-X is motivated such as in the TeV scale model of neutrino, dark matter, and baryogenesis. In the Type-X, b→sγ bound is very mild. →Light charged Higgs scenario is possible. By measuring single A/H production (LHC) and AH +, HH +, AH production (LHC and ILC), one could test the Type-X THDM. ・ Extended Higgs models ⇔ New physics

21. b→sγ Type-I, X Type-II, Y t s b γ W－W－ H－H－ γ bts In the Type-X THDM, destructive interferences occur between the W and the H ± contributions. Barger, Hewett, Phillips PRD 41 (1990)

23. B→τν Type-X no bound τ→μνν If m H+ >100GeV, then tanβ=60 is allowed :Type-II :Type-X Aoki, Kanemura, Tsumura, K.Y arXiv:0902.4665 [hep- ph] Krawczyk, Sokolowska arXiv:0711.4900 [hep-ph] D.s.Du arXiv:0709.1315 [hep-ph]